1/158
Looks like no tags are added yet.
Name | Mastery | Learn | Test | Matching | Spaced |
---|
No study sessions yet.
electic current (I)
I= ΔQ/Δt
units C/s or A
ohm’s law
V=IR
power dissipated by resistor
P= IV=V2/R=I2R=Energy/t
resistance (R)
R=(ρL)/A
kirchoff’s rules
ΣV=0 (loop rule)
ΣIin=Iout (junction rule)
capacitator charge
Q=CV
dielectrics and capacitors equations
energy stored in capacitors
Uc=1/2QV=1/2C(V)2=1/2(Q2/C)
resistors in series and parallel
polarization
the separation of positive and negative charges within an object
what is the difference between conductors and insulators?
conductors allow charges to move through them easily while insulators do not
law of conservation of electric charge
total electric charge in an isolated system is constant
coulomb (C) or elementary charge (e)
1.60 × 10-19
couloumbs law
electrostatic force between two charged particles
k= constant of proportionality= 9 × 109 Nm2/C2
magnitude of electric field
r= distance between source and test charge
which direction does an electric field point?
the electric field vectors point AWAY from POSITIVE charges and TOWARDS NEGATIVE charges
properties of electric field charges
direction from + charge towards - charge
number of field lines drawn ansd closeness of lines indicates strength of the field
electric field vs electrostatic force on a charge within the field equation
electric potential
the energy needed to move a charge in an electric field from one point to another
equipotential lines
indicate the electric potential at any given point around a charge in an electric field
electric potential energy (withina. field)
energy stored in a charged object due to its position within an electric field
change in electric potential energy between two points
work done by an electric field
amount of electric potential energy that is changed (dependent only on the initial and final locations of the potentials)
W>0 charge moves in the direction of electric field (higher to lower potential)
W<0: charge moves opposite direction of electric field (low to high potential)
electric potential energy (between two charges)
electric field strength
prefixes and symbols for 1012 to 1012
1012: Tera (T)
109: Giga (G)
106: Mega (M)
103: Kilo (k)
10-2: Centi ©
10-3: Mili (m)
10-6: Micro (μ)
10-9: Nano (n)
10-12: Pico (p)
sin, cos, tan of 0
sin: 0
cos: 1
tan: 0
sin, cos, tan of 30
sin: 1/2
cos: √3/2
tan: √3/3
sin, cos, tan 37
sin: 3/5
cos: 4/5
tan: 3/4
sin, cos, tan 45
sin: √2/2
cos: √2/2
tan: 2
sin, cos, tan 53
sin: 4/5
cos: 3/5
tan: 4/3
sin, cos, tan 60
sin: √3/2
cos: 1/2
tan: √3
sin, cos, tan 90
sin: 1
cos: 0
tan: infinity
proton mass (mp)
mp=1.67 × 10-27 kg
neutron mass (np)
mn=1.67 × 10-27 kg
electron mass (me)
me= 9.11 × 10-31 kg
electron charge magnitude
e=1.6 × 10-19 C
1 electron volt
1 ev=1.6 × 10-19 C
speed of light ©
c= 3 × 108 m/s
universal gravitational constant
G= 6.67 × 10-11 m3/(kg x s2)
acceleration due to gravity at Earth’s surface
g=10 m/s2
avogadro’s number
NA=6.02 × 1023 mol-1
universal gas constant (2 kinds!)
R= 8.314 J/mol x K
R= 0.0821 L atm/ mol K
boltzmann’s constant
KB= 1.38 × 10-23 J/k
relationship between L x Pa and J
1 L x Pa = 0.001 J
relationship between L and m
1 L= 0.001 m3
relationship between cm3 and m3
1 cm3= 1 × 10-6 m3
examples of vector quantities
displacement
velocity
acceleration
force
torque
momentum
electric field
weight
examples of scalar quantities
distance
speed
work/energy
power
presure
electric potential
temperature (but can be positive or negative)
density
mass
displacement equations
Δx=vi(t)
Δx= Δx0 + vi(t) + 1/2a(t)2
final velocity equations
vf=vi+ a(t)
(vf)2=(vi)2 + 2aΔx
displacement
average velocity
vavg= (vi+vf)/2
projectile horizontal displacement
Δx= vi,x(t)
projectile max height
Hmax= (vi,y)2/2g
projectile max range
R= ((vi)2 (sin 2θ))/g
projectile total flight time
t= 2vi,y/g
net force
Fnet=ma
newton’s 3rd law
-F1=F2
friction
f=μFN
static friction
fs</= μsFN
kinetic friction
fk= μkFN
tension of two blocks connected by a rope
SAME
torque
τ=rFsinθ
+= CCW
-= CW
critical point
point where center of gravity is no longer directly above the base of support
stable equilibrium
if displaced, returns back to original position (cg remains within the base of support)
unstable equilibrium
if displaced, it does not return to its original position (cg is outside the base of support)
neutral equilibrium
if displaced, it remains in its new positio (such as a ball placed on a horizontal position)
static equilibrium
state of equilibrium where an object is at rest
dynamic equilibrium
state of equilibrium where an object is moving at constant velocity
x-component of force
Fx=Fcosθ
y-component of force
Fy=Fsinθ
magnitude of force
F= √(Fx)2+(Fy)2
unknown angle of force
tanθ= Fy/Fx
weight
Fg=mg
kinetic energy
KE=(1/2)mv2
linear momentum
p=mv
impulse
Δp=FΔt
kinetic energy/work theorem
Wnet=ΔKE=(1/2)mvf2-1/2)mvi2
W=F||d=Fdcosθ
power
P=ΔE/Δt=W/t=Fv
center of mass
xcm=Σmixi/Σmi
mechanical energy
E= KE + UG
gravitational potential energy
UG= mgh
conservation of mechanical energy
ΔE= ΔKE + ΔU = -Wfr
efficiency
e=Wout/Ein
hooke’s law
Fx=-kx
spring potential energy
U=(1/2)kx2
period of simple harmonic oscillator
Ts= 2π√m/k
frequency of simple harmonic oscillator
f=1/2π√k/m
angular frequency
ω=2π/T=√k/m=2πf
max speed of a spring
vmax= Aω
max acceleration of a spring
amax=Aω2
period of a simple pendulum
Tp= 2π√L/g
frequency of a simple pendulum
f=1/2π√g/L
position of simple harmonic motion
x=Acos(ωt)=Acos(2πft)
wavelength
λ=v/f
malus law
I=I0cos2θ
intensity of sound
dB=10log10(Ii/I0)
frequency of string attached at both ends
f= nv/2L
frequency of pipe open at both ends
f= nv/2L
frequency of pipe open at one end
f= nv/4L
*note: harmonics is odd numbers